EP1146386A1 - Nichtblockierender Freiraumschalter - Google Patents

Nichtblockierender Freiraumschalter Download PDF

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Publication number
EP1146386A1
EP1146386A1 EP00810326A EP00810326A EP1146386A1 EP 1146386 A1 EP1146386 A1 EP 1146386A1 EP 00810326 A EP00810326 A EP 00810326A EP 00810326 A EP00810326 A EP 00810326A EP 1146386 A1 EP1146386 A1 EP 1146386A1
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EP
European Patent Office
Prior art keywords
switch
output
input
free space
tunable
Prior art date
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Withdrawn
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EP00810326A
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English (en)
French (fr)
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EP1146386A8 (de
Inventor
Folkert Horst
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International Business Machines Corp
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International Business Machines Corp
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Publication date
Application filed by International Business Machines Corp filed Critical International Business Machines Corp
Priority to EP00810326A priority Critical patent/EP1146386A1/de
Priority to TW090102789A priority patent/TW499587B/zh
Priority to CA002404951A priority patent/CA2404951C/en
Priority to AU35914/01A priority patent/AU3591401A/en
Priority to JP2001576533A priority patent/JP3914436B2/ja
Priority to PCT/IB2001/000328 priority patent/WO2001079926A1/en
Priority to KR10-2002-7013306A priority patent/KR100488847B1/ko
Publication of EP1146386A1 publication Critical patent/EP1146386A1/de
Publication of EP1146386A8 publication Critical patent/EP1146386A8/de
Priority to US10/268,640 priority patent/US6813409B2/en
Withdrawn legal-status Critical Current

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    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/29—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
    • G02F1/295—Analog deflection from or in an optical waveguide structure]
    • G02F1/2955—Analog deflection from or in an optical waveguide structure] by controlled diffraction or phased-array beam steering
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122—Basic optical elements, e.g. light-guiding paths
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B2006/12133—Functions
    • G02B2006/12145—Switch
    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/0147—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on thermo-optic effects
    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/29—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the position or the direction of light beams, i.e. deflection
    • G02F1/31—Digital deflection, i.e. optical switching

Definitions

  • the invention concerns an optical switch, and in particular a non-blocking free-space switch.
  • Optical switches very much like the conventional transistor, are essential components of photonic guided-wave devices. Optical switching is needed for rearranging the optical paths in a telecommunication network, for example.
  • optical switches have one or more elements that are mechanically actuated. These kind of switches are thus referred to as optomechanical switches. Typical examples are addressed in "Current European WDM deployment trends", E. Lowe, IEEE Commun. Mag., Vol. 36, pp. 46-50, 1998, and in “All-silicon bistable micro mechanical fiber switches", M. Hoffmann et al., Electron. Lett., Vol. 34, pp. 207-208, 1998.
  • a second approach, which uses beam-steering to realize a 1xN or Nxl switch is described in "Compact Versatile Thermooptical Space Switch Based on Beam Steering by a Waveguide Array", E. peck et al., IEEE Photonics Techn. Lett., Vol. 11, No. 11, pp. 1399-1401, November 1999.
  • This integrated optical switch resembles known arrayed waveguide grating (AWG) wavelength multiplexers. It consists of a number of input waveguides, a star coupler that divides the input light over an array of channel waveguides and a second star coupler that refocuses the light from the array onto one of the output waveguides.
  • the array waveguides at the input side are equipped with tunable lenses. By adjusting the phase distribution one can determine onto which output waveguide the light is focussed. This allows to switch input signals to desired output channels.
  • This IEEE publication is herewith incorporated by reference.
  • a switch in accordance with the present invention, comprises an input channel with an input optical free space element, a large optical free space element, an input tunable optical lens with adjustable projection characteristic for projecting a light wave received from the input optical free space element into the large free space element.
  • the switch comprises an output channel with an output optical free space element, and an output tunable optical lens with adjustable receiving characteristic for capturing the light wave from the large free space element and for feeding the light wave to the output optical free space element.
  • the present switch can be implemented in various material systems including Silicon oxinitride (SiON), III-V semiconductors like InP, silica (i.e., SiO 2 ) glasses, lithiumniobate, and polymers.
  • SiON Silicon oxinitride
  • III-V semiconductors like InP
  • silica (i.e., SiO 2 ) glasses lithiumniobate
  • polymers polymers
  • An optical waveguide usually comprises a core made of some high-refractive index material and a cladding of a low-refractive index material.
  • the core and cladding may be made of doped silica glass, where the necessary refractive index contrast is achieved by an appropriate doping profile.
  • a semiconductor technology compatible substrate such as a Si wafer (e.g., a four inch Si wafer), or on a glass substrate. This results in what is called a planar waveguide or an integrated planar waveguide.
  • the cladding is made of silica, which has a refractive index of 1.45
  • a material with a higher refractive index e.g., near 1.5
  • SiON can be chosen for the core, because its refractive index can be tuned over a wide range by changing the nitrogen concentration of the material.
  • An example for use of SiON as waveguide is described in US patent 5,416,861.
  • a particular feature of SiO x N y resulting from a mixture of the components SiO 2 and Si 3 N 4 is that it forms amorphous structures and that the components are miscible over the whole possible range.
  • a typical composition of the waveguide core is SiO 1.9 N 0.08 .
  • a known fabrication technique is to deposit SiON using a Plasma Enhanced Chemical Vapor Deposition (PECVD) process.
  • PECVD Plasma Enhanced Chemical Vapor Deposition
  • the resulting material has, however, a large hydrogen concentration.
  • Hydrogen is incorporated in the form of hydroxyl groups, Si-H groups and NH- and NH 2 -fragments. These groups and fragments introduce additional absorption into the optical transmission characteristic of the silicon oxinitride.
  • the first overtone of the NH-induced absorption band lies at 1505 nm and overlaps with the spectral window, which is used for optical signal transmission and which extends from 1540 nm to 1570 nm, hereinafter simply referred to as the optical transmission window.
  • This window has been chosen for optical transmission due to the fact that silica glass there has its lowest absorption and that erbium-doped optical amplifiers there have the range of most linear amplification as can be read upon in "Review of rare earth doped fiber lasers and amplifiers" by P.Urquhart, IEE Proc. Vol. 135, Pt. J, No. 6, pp 385-407, December 1988.
  • waveguide array is meant to refer to an array of channel waveguides. Ridge waveguide (also called stripe waveguide) structures, buried waveguide structures and any other structure is well suited for use in connection with the present invention.
  • array waveguides a number of different shapes and geometry can be applied. Note that in the Figures for sake of simplicity only waveguide arrays with straight waveguide channels are shown. In most practical applications these waveguide channels are bent, as shown in Figure 9, for example.
  • the word channel refers to one particular link of a communication link that carries a multiwavelength light wave.
  • An optical free space element has a free propagation region where light is not laterally confined. Light can be projected from an input waveguide (herein referred to a input channel) or input waveguide array into such an optical free space element.
  • Optical free space elements are in the literature also referred to as free propagation regions (FPRs).
  • FPRs free propagation regions
  • a “tunable lens”, as herein used, comprises a waveguide array plus phase shifters (e.g., heaters).
  • This tunable lens takes a divergent or parallel beam propagating in a first optical free space element (e.g., an input optical free space element) and transforms this beam into a parallel or convergent beam in a second optical free space element, just like a normal lens would do.
  • a first optical free space element e.g., an input optical free space element
  • transforms this beam into a parallel or convergent beam in a second optical free space element just like a normal lens would do.
  • everything between the first optical free space element and the second optical free space element makes up the tunable lens.
  • the focusing properties of the waveguide array and the wavelength dependency are determined by the relative effective optical lengths of the waveguides in the waveguide array.
  • This effective optical length is determined by the effective index of refraction and the physical length of the waveguide. It can be fine-tuned using the phase shifters (e.g., heaters).
  • a tunable lens can be implemented in different manners.
  • a typical example is a tunable lens that comprises an individually tunable heater for some or all of the waveguides of a waveguide array. Under certain circumstance it is desirable to employ more than one heater per waveguide.
  • a linear phase gradient leads to a tilting (steering) of the phase front of the light emitted.
  • quadratic or higher order phase gradients one can change the focal distance of the light wave. In other words, such a tunable lens allows a thermooptical control of the projection characteristic.
  • Such a heater steering unit may comprise a microcomputer and a memory to store the respective heater settings, or it may be connected to a switch control box or a computer (e.g., via a computer interface).
  • a switch control box obtains/extracts routing or switching information (connection information) either from the packets or frames received on the input side of the switch, or this connection information is received from other systems. The respective connections are then established inside the switch/optical chip via the heater steering unit and the input- and output tunable lenses.
  • Micromechanical on-chip elements can also be used to realize a tunable lens.
  • the basic elements of a switch are: an input optical free space element, an input tunable lens, a large optical free space element, an output tunable lens, and an output optical free space element.
  • the path for a connection through the switch is as follows: light from an input channel is launched into an input optical free space element and becomes a laterally divergent beam. This divergent beam is picked up by the first tunable lens (waveguide array plus heaters) and transformed into a parallel or convergent beam in the large optical free space element. At the end of this large optical free space element the beam is still parallel, or divergent again (past the focal point). This parallel or divergent beam is picked up by the second tunable lens (second waveguide array plus heaters) and transformed into a convergent beam in the output optical free space element. The position of the focal point in this element is adjusted such that it coincides with the start of the output waveguide. The light is then coupled into this output waveguide and leaves the switch through it.
  • the NxN switching functionality is obtained by adjusting the input tunable lens to steer the direction of the beam in the large optical free space element. For a number of different settings, this beam can be pointed into the direction of a number of different output tunable lenses. In the same way, the output tunable lenses can be adjusted such that for a number of different settings, beams coming from different input tunable lenses are projected onto the waveguides of the output waveguide arrays.
  • the focal length of the input tunable lens P is set to transmit a convergent beam with a focal point in the large optical free space element half-way between the input and the output tunable lenses, and the output tunable lens Q is set to refocus the divergent beam after this focal point onto the output waveguide.
  • Important optical properties of the switches according to the present invention are the transmission loss, output channel loss uniformity, channel isolation, etc. Given a fixed waveguide technology, the free design parameters that can be used to adjust properties of the switch are well known and understood by a person of skill in the art. Analytical as well as numerical modeling or simulation tools can be used when designing a switch according to the present invention. This procedure follows the same considerations as applied when modeling standard AWG devices.
  • FIG. 1F An exemplary cross-section of a waveguide with a ridge structure is shown schematically in Figure 1F.
  • a Si substrate 20 e.g., a Si wafer
  • a SiO 2 layer 21 also referred to as lower cladding
  • aSiON core 22 is grown by using a PECVD process.
  • the result of this PECVD step is illustrated in Figure 1B.
  • the whole structure 20, 21, 22 may now be annealed in an annealer to reduce absorption losses caused by N-H bonds.
  • a Tempress System TS-6304 can be used as annealer.
  • a ridge 23 is now defined by means of a Reactive Ion Etching (RIE) process.
  • RIE Reactive Ion Etching
  • This ridge 23 is supposed to serve as waveguide channel.
  • an upper cladding layer 24 is formed on top of the SiON core 22 and ridge 23.
  • the upper cladding layer 24 comprises SiO 2 that was deposited using PECVD.
  • Figure 1D illustrates a waveguide after this upper cladding layer 24 was deposited.
  • a chromium heater for example.
  • additional steps are illustrated in Figures 1E - 1F.
  • a chromium layer 25 is deposited on the upper cladding layer 24 so that it covers part of the.
  • a sputter deposition process can be used to form the chromium layer 25.
  • An additional aluminum layer 26 can be deposited by sputtering to form a low-resistance contact line. This is illustrated in Figure 1F.
  • a typical waveguide has a ridge width between 1 ⁇ m and 5 ⁇ m, preferably 3 ⁇ m, and a thickness between 1 ⁇ m and 3 ⁇ m, preferably of 1.3 ⁇ m.
  • the original thickness of the SiON layer 22 ( Figure 1B) is between 1 ⁇ m and 5 ⁇ m, and preferably about 2 ⁇ m. After the ridge formation this layer 22 is reduced to a thickness of about .65 ⁇ m ( Figure 1C).
  • the SiO 2 cladding layers 21 and 24 have a refractive index of about 1.45 and the SiON core 22 has a refractive index of about 1.5. The index contrast is thus about 3.3%.
  • the present waveguides have a propagation loss of less than 0.15 dB/cm.
  • waveguides can be realized that have a relatively small geometrical cross-section and a high lateral effective refractive-index contrast of 0.02 compared to standard single mode fibers.
  • the tunable lens 40 comprises a waveguide array 39 with three ridge waveguides 30, 31, and 32. The light is channeled along these waveguides from left to right.
  • Two chromium heaters 25 and 35 are arranged on top of the two uppermost waveguides 30, 31.
  • the two heaters 25, 35 are connected by a first aluminum contact line 26 to a first contact pad 36.
  • This first aluminum contact line 26 serves as a common electrode.
  • Each of the two heaters 25, 35 also has its individual aluminum contact line 42, 43 and contact pad 37, 38. This arrangement of aluminum contact lines allows to individually drive current (I1, I2) through the two heaters 25, 35.
  • a steering unit 44 can be employed that drives the individual heaters.
  • These heaters 25, 35 are part of the tunable lens 40 that allows to adjust the phase gradient across the different waveguides. By adjusting the phase gradient one can control the projection characteristic of the light emitted by the waveguide array 39 into a large optical free space element (not shown in Figure 2A).
  • FIG. 2B An exemplary top-view of an input optical free space element 180 is schematically illustrated in Figure 2B.
  • the input optical free space element 180 has one input channel 181 which guides a multiwavelength light wave towards the input optical free space element's free propagation region.
  • the light wave diverges, as indicated in Figure 2B by the four lines with arrows.
  • This divergent beam is picked up by the four waveguide channels 182 - 185 of the waveguide array 186.
  • This waveguide array 186 is part of a tunable lens (not shown in this Figure 2B).
  • An output optical free space element 190 is schematically illustrated in Figure 2C.
  • This element 190 comprises a waveguide array 196 with four channel waveguides 192 - 195, a free propagation region, and an output channel 191.
  • a parallel or divergent beam - schematically represented by four lines with arrows - transforms by superposition into a convergent beam in the output optical free space element 190 if the phase relations in the waveguides of the waveguide array 196 are set correctly. The convergent beam is then coupled into this output channel 191.
  • FIG. 3A shows the switch 10 in a first switching state (on-state) where the input side is connected to the output side.
  • first switching state on-state
  • second switching state off-state
  • the connection between the waveguide 6 at the input side and the waveguide 7 at the output side is interrupted and no coupling between the two sides takes place.
  • This second state is illustrated in Figure 3B.
  • the switch 10 comprises three optical free space elements: an input optical free space element 8, a large optical free space element 13, and an output optical free space element 9.
  • the switch 10 comprises an input tunable optical lens 12 with an input waveguide array 11, and an output tunable optical lens 15 with an output waveguide array 14.
  • the input optical free space element 8 sits in front of this input tunable optical lens 12 and the output optical free space element 9 follows after the output tunable optical lens 15.
  • a light wave 16 arriving via the input waveguide 6, the input optical free space element 8, and the input waveguide array 11 with input tunable optical lens 12 is projected into the large optical free space element 13.
  • the input tunable optical lens 12 interacts with the input waveguide array 11 such that the light wave 16 in the large free space element 13 can be steered by adjusting the lens 12. Due to the adjustment of the lens 12 one can change the projection characteristic of the input tunable optical lens 12.
  • the input tunable optical lens 12 is adjusted such that the light wave 16 has a focal point 17 right in the middle of the large free space element 13.
  • the output tunable optical lens 15 is arranged such that it is able to receive the light wave 16 from the large free space element 13, provided that its receiving characteristic is adjusted accordingly.
  • the output tunable optical lens 15 comprises an output waveguide array 14 and heaters that allow to adjust the receiving characteristic so as to (actively) capture the light wave 16 from the large free space element 13.
  • all light from the input waveguide array 11 is focussed at focal point 17 and from there captured by the output waveguide array 14.
  • the output optical free space element 9 collects the light from the waveguide array 14 into the output channel 7.
  • the same switch 10 is shown in a second state, also referred to as off-state. It is obvious that there are various other switching states.
  • the input tunable optical lens 12 is adjusted such that the light wave 16 has a focal point 19 that is not in the middle of the large free space element 13 anymore.
  • the light wave 16 was tilted upwards by tuning the input tunable optical lens 12.
  • the output tunable optical lens 15 has not been adjusted in the present example which means that the receiving characteristic remains the same.
  • the output tunable optical lens 15 has a focal point 18. Since the focal points 18 and 19 are spaced apart, there is no (or almost no) light coupled from the input side to the output side. This explains why this state is also called off-state.
  • a switch in accordance with the one illustrated in Figures 3A and 3B can be used to realize an on/off switch.
  • This switch 50 is an NxN free-space non-blocking switch. It comprises N input channels 187, 188, 189, each having a (small) input optical free space element 181, 182, 183, and an input tunable optical lens 54, 55, 56 with input waveguide arrays 51, 52, 53.
  • the switch 50 furthermore comprises a large free space element 60, and N output channels 190, 191, and 192.
  • Each output channel has an output tunable optical lens 61, 62, 63 with output waveguide arrays 57, 58, 59 and a (small) output optical free space element 184, 185, 186.
  • the tunable optical lenses 54, 55, 56 on the input side and the tunable optical lenses 61, 62, 63 on the output side are adjusted such that a light wave 64 arriving via the input waveguide array 51 is focussed onto focal point 67 and then captured by the output waveguide array 58.
  • the light wave 65 is emitted by the input waveguide array 52 into the large free space element 60 and projected onto the focal point 69.
  • the output waveguide array 59 captures the light wave 65.
  • the light wave 66 emitted by the N-th input waveguide array 53 is focused onto the focal point 68.
  • the output waveguide array 57 captures this light wave.
  • a switch 70 is shown that comprises N input channels 74 - 76, N input optical free space elements 71 - 73, and N tunable lenses 152 - 154 with N input waveguide arrays.
  • the switch further comprises a large optical free space element 151.
  • the switch 70 comprises N output channels 81 - 83, N output optical free space elements 77 - 79, and N tunable lenses 155 - 157 with N output waveguide arrays.
  • a filtering element 80 is placed in the middle of the free space element 151. This filtering element 80 sits where the intermediate focal plane of the switch 150 is. It comprises openings at those locations where focal points are.
  • the input waveguide arrays create a real image of the input waveguides in the middle of the large free space element 151 exactly where the openings of the filtering element 80 are.
  • the arrays at the output side can be tuned to actively capture light from those openings. Any higher order diffraction peaks from the waveguide arrays that hit the filtering element 80 outside the openings is suppressed by the filtering element 80.
  • the filtering element 80 serves as an optical filter.
  • the positions of real images in this intermediate focal plane can be calculated. In case of an NxN switch there are 2xN-1 focus points, i.e., the filtering element 80 would have 2xN-1 openings.
  • Each output channel comprises a tunable lens 206 with five waveguides 95 and an output free space element 194.
  • the waveguides 91 and 95 are arranged with respect to the large free space element 92 such that (1) the focal points all are on the focal plane 93, and (2) such that the focal plane is in the middle of the large free space element 92.
  • the present symmetrical switch arrangement has tunable lenses, like the other switches addressed before.
  • Figure 6 represents a switch state where all tunable lenses are in their off-state, i.e., no beam steering takes place.
  • the switch routes a first light wave from the uppermost input channel 120 to the uppermost output channel 123.
  • a second light wave is routed from the input channel 121 in the middle to the output channel 124 in the middle, and a third light wave is routed from the input channel 122 at the bottom to the output channel 125 at the bottom.
  • This switch 90 can now be switched into various switch states by adjusting the input tunable optical lenses and/or the output tunable optical lenses. Let us assume for the time being that just the input tunable optical lens of the uppermost input channel 120 is adjusted in order to move the focal point of the uppermost light beam upwards. With all the other tunable optical lenses in the off-states this would mean that the focal point of the uppermost input channel 120 and the uppermost output channel 123 do not coincide anymore. The first light wave arriving via this channel 120 is not routed to the output channel 123. This particular optical 'link' is interrupted.
  • the tunable lenses 207, 208 are arranged with respect to the large free space element 132 such that (1) the focal points all are on the focal plane 133, and (2) such that the focal plane 133 is in the middle of the large free space element 132.
  • the present switch arrangement 130 has tunable lenses 207 and 208, like the other switches addressed before.
  • these tunable lenses 207, 208 are only schematically depicted in Figure 7. All tunable lenses 207, 208 are in their off-state, i.e., no beam steering takes place.
  • the light beams enter the large free space element 132 and are focussed onto focal points 134.
  • the receiving characteristic of the output tunable lenses 208 is adjusted such that the focal points 136 do not overlap with the focal points 134.
  • no light is captured by the output tunable lenses 208, i.e., the input channels 140, 141, 142 are not coupled to any of the output channels 143, 144, 145. No light travels from the left hand side to the right hand side.
  • the optical links are all interrupted.
  • This switch 130 can now be switched into various switch states by adjusting the input tunable optical lenses 207 or the output tunable optical lenses 208.
  • both the input tunable optical lenses 207 and the output tunable optical lenses 208 are adjusted so as to satisfy the criteria a) - c) for an optimal link, as defined in an earlier section of the detailed description.
  • the switches 90 and 130 both can be switched by adjusting the beam direction in the large free space element.
  • the large free space element 161 has a reflective surface 162.
  • a first light wave arriving via the input channel 201 is focused onto the reflective surface 162 from where it is captured by the output channel 203.
  • a second light wave arriving via the input channel 202 is focused onto the reflective surface 162 from where it is captured by the output channel 204.
  • Such a switch 160 may require less space than the other switches presented herein since the size of the large free space element 161 can be reduced.
  • This switch 210 is characterized in that its input side is a mirror image of its output side.
  • the switch 210 comprises 8 input channels 212, followed by 8 input optical free space elements 213, and 8 input tunable lenses 214 with heaters and waveguide arrays.
  • the waveguides of these waveguide arrays are connected/coupled to a large optical free space element 211.
  • On the opposite side of the free space element 211 there are 8 output tunable lenses 215 with heaters and waveguide arrays. These 8 output tunable lenses 215 feed light into 8 output optical free space elements 216 that are coupled to 8 output channels 217. Note that the contact lines for the individual heaters are not shown in Figure 9.
  • the switch 210 is made using IBM's high-index-contrast silica-on-silicon integrated planar waveguide technology.
  • the preferred dimensions for switch 210 are given on the top left-hand side of Figure 9.
  • the input channels 212 and the output channels 217 are separated by 0.1 mm through 0.5 mm, and preferably by about 0.25 mm
  • the 8 input optical free space elements 213 and the 8 output optical free space elements 216 each have a length of 1 mm through 0.1 mm, preferably about 0.5 mm, and a width of 1mm through 0.1 mm, preferably 0.3 mm.
  • the large optical free space element 211 has a length of 10 mm through 1 mm, preferably about 4 mm, and a width of 10 mm through 0.5 mm, preferably 2.4 mm.
  • the separation of the waveguides at the optical free space elements 213, 11, and 216 is between 1 ⁇ m and 20 ⁇ m, preferably about 8 ⁇ m.
  • the heater pads or lines have a length between 1 mm and 10 mm, preferably about 2 mm.
  • the pads are separated between 50 ⁇ m and 500 ⁇ m, preferably by about 100 ⁇ m.
  • the separation of the individual heater arrays is between 100 ⁇ m and 0.1 mm, preferably about 400 ⁇ m.
  • IBM's high-index-contrast silica-on-silicon integrated planar waveguide technology allows to make waveguides with small bending radii and the switch design can be further optimized to reduce the lateral size.
  • the heater steering unit may comprise a unit that allows the adjustment of the power in the output channel.
  • the number of input channels does not have to be equal to the number of output channels.
  • the number of waveguides per waveguide array does not have to be the same on the input side and output side. It is also conceivable that there are a few input channels with five waveguides and a few input channels with six waveguides, for example.
  • the present switch may comprise one or more coupling elements.
  • a v-shaped groove for example, may serve as a coupling element. Such an element allows the butt-coupling of a fiber to one of the input channels or output channels.
  • the present switch is well suited for integration with a large number of other components on a chip.
  • the switches, according to the present invention provide the high functionality which will be required by future telecommunication networks.
  • the present invention can be integrated into multiwavelength telecommunication data transmission systems.
EP00810326A 2000-04-14 2000-04-14 Nichtblockierender Freiraumschalter Withdrawn EP1146386A1 (de)

Priority Applications (8)

Application Number Priority Date Filing Date Title
EP00810326A EP1146386A1 (de) 2000-04-14 2000-04-14 Nichtblockierender Freiraumschalter
TW090102789A TW499587B (en) 2000-04-14 2001-02-08 Tree-space non-blocking switch
CA002404951A CA2404951C (en) 2000-04-14 2001-03-02 Free-space non-blocking switch
AU35914/01A AU3591401A (en) 2000-04-14 2001-03-02 Free-space non-blocking switch
JP2001576533A JP3914436B2 (ja) 2000-04-14 2001-03-02 自由空間ノンブロッキング・スイッチ
PCT/IB2001/000328 WO2001079926A1 (en) 2000-04-14 2001-03-02 Free-space non-blocking switch
KR10-2002-7013306A KR100488847B1 (ko) 2000-04-14 2001-03-02 광학 스위치
US10/268,640 US6813409B2 (en) 2000-04-14 2002-10-10 Free-space non-blocking switch

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
EP00810326A EP1146386A1 (de) 2000-04-14 2000-04-14 Nichtblockierender Freiraumschalter
US10/268,640 US6813409B2 (en) 2000-04-14 2002-10-10 Free-space non-blocking switch

Publications (2)

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EP1146386A1 true EP1146386A1 (de) 2001-10-17
EP1146386A8 EP1146386A8 (de) 2002-01-02

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US (1) US6813409B2 (de)
EP (1) EP1146386A1 (de)
JP (1) JP3914436B2 (de)
AU (1) AU3591401A (de)
CA (1) CA2404951C (de)
TW (1) TW499587B (de)
WO (1) WO2001079926A1 (de)

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US20080019640A1 (en) * 2006-03-03 2008-01-24 Robert Blum Dynamically tunable waveguide chip for optical transforms
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KR101803326B1 (ko) * 2012-03-14 2017-12-04 한국전자통신연구원 광 스위치 소자 및 그 제조방법
US20140305910A1 (en) * 2013-03-27 2014-10-16 Ipg Photonics Corporation System and Method Utilizing Fiber Lasers for Titanium Welding Using an Argon Cover Gas
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EP1636620B1 (de) * 2003-06-19 2010-06-09 Polatis Ltd Verbesserung eines optischen schalters mit strahlsteuerung
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US20040071390A1 (en) 2004-04-15
JP3914436B2 (ja) 2007-05-16
US6813409B2 (en) 2004-11-02
CA2404951A1 (en) 2001-10-25
JP2003531399A (ja) 2003-10-21
TW499587B (en) 2002-08-21
EP1146386A8 (de) 2002-01-02
AU3591401A (en) 2001-10-30
CA2404951C (en) 2007-09-04
WO2001079926A1 (en) 2001-10-25

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